Coherent Backscattering from Multiple Scattering Systems - KOPS ...
Coherent Backscattering from Multiple Scattering Systems - KOPS ...
Coherent Backscattering from Multiple Scattering Systems - KOPS ...
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5.1 Conservation of energy in coherent backscattering<br />
1<br />
kl* = 2<br />
kl* = 4<br />
kl* = 10<br />
0.8<br />
cooperon<br />
0.6<br />
0.4<br />
0.2<br />
0<br />
−90 −60 −30 0 30 60 90<br />
scattering angle [deg]<br />
Figure 5.5: Old and new theory. The graph shows the cooperon calculated with<br />
eqn. 2.15 (dashed lines) and including the additional contribution given in eqn. 5.7<br />
(solid lines). The dotted lines give the enhancement of the cooperon for the new theory<br />
(for the old theory the enhancement is always equal to 1). Parameters: wavelength<br />
λ = 590 nm, diffusion coefficient D = 15 m2 /s, reflectivity R = 0.5.<br />
The fit parameter a is therefore obtained by numerical integration of<br />
a =<br />
0<br />
∫ π/2<br />
0<br />
∫ π/2<br />
I (A)<br />
c<br />
1<br />
(kl ∗ ) 2 ·<br />
· sin θ dθ<br />
µ · sin θ dθ<br />
µ + 1<br />
After normalization analogous to eqns. 2.13, the additional contribution to the cooperon finally<br />
becomes<br />
α (B+C)<br />
c<br />
8π · a<br />
= −<br />
3 k 2 l ∗ (l ∗ + 2z 0 ) ·<br />
µ<br />
µ + 1<br />
(5.7)<br />
does not contribute at a specific angular value but it is rather spread out over the<br />
whole angular range, similar to the diffuson. In particular it reduces the enhancement of the<br />
coherent backscattering cone, so that the total cooperon α (A)<br />
c<br />
α (B+C)<br />
c<br />
+ α (B+C)<br />
c at the conetip at θ = 0<br />
51